Bipolar Junction Transistor (BJT)aries.ucsd.edu/.../ECE65/12-W/Slides/ECE65_W12-BJT.pdf · A BJT consists of three regions F. Najmabadi, ECE65, Winter 2012 Simplified physical structure.

Bipolar Junction Transistor (BJT)

Lecture notes: Sec. 3

Sedra & Smith (6th Ed): Sec. 6.1-6.4* Sedra & Smith (5th Ed): Sec. 5.1-5.4*

* Includes details of BJT device operation which is not covered in this course

F. Najmabadi, ECE65, Winter 2012

A BJT consists of three regions


Simplified physical structure

NPN transistor An implementation on an IC

Device construction is NOT symmetric o “Thin” base region (between E & C) o Heavily doped emitter o Large area collector

Device is constructed such that BJT does NOT act as two diodes back to back (when voltages are applied to all three terminals).

Six circuit variables: (3 i and 3 v) Two can be written in terms of the

other four:

BJT iv characteristics includes four parameters


NPN transistor

CEBEBC

BCE

vvviii−=

+= :KVL

:KCL

Circuit symbol and Convention for current directions

(Note: vCE = vC – vE)

BJT iv characteristics is the relationship among (iB , iC , vBE , and vCE )

It is typically derived as ),(

)(

CEBC

BEB

vi givfi

==

Active mode:

0

/

/

DCE

VvSC

VvSCB

VveIi

eIii

TBE

TBE

≥=

==ββ

BJT operation in the “active” mode


If the base is “thin” these electrons get near the depletion region of BC junction and are swept into the collector if vCB ≥ 0 (vBC ≤ 0 : BC junction is reverse biased!)

In this picture, ic is independent of vBC

(and vCE ) as long as

TBE VvSC eIi /=

0

0 0

DCE

CEDCEBEBC

VvvVvvv

≥≤−=−=

As Emitter is heavily doped, a large number of electrons diffuse into the base (only a small fraction combine with holes) The number of these electrons scales as TBE Vve /

BE junction is forward biased (vBE = VD0)

Base current is also proportional to

and therefore, iC : iB = iC/β

TBE Vve /

BJT operation in saturation mode


For vBC ≥ 0 BC junction is forward biased and a diffusion current will set up, reducing iC .

1. Soft saturation: vCE ≥ 0.3 V (Si)* vBC ≤ 0.4 V (Si), diffusion current is small and iC is very close to its active-mode level.

2. Deep saturation region: 0.1 < vCE < 0.3 V (Si) or vCE ≈ 0.2 V = Vsat (Si), iC is smaller than its active-mode level (iC < β iB). o Called saturation as iC is set by outside

circuit & does not respond to changes in iB.

3. Near cut-off: vCE ≤ 0.1 V (Si) Both iC & iB are close to zero.

Similar to the active mode, a large number of electrons diffuse into the base.

BE junction is forward biased (vBE = VD0)

“Deep” Saturation mode:

satCE

BC

VvSB

Vvii

eIi TBE

≈<

=

/

ββ

* Sedra & Smith includes this in the active region, i.e., BJT is in active mode as long as vCE ≥ 0.3 V.

BJT iv characteristics includes four parameters


NPN transistor

Circuit symbol and Convention for current directions

(Note: vCE = vC – vE)

BJT iv characteristics is the relationship among (iB , iC , vBE , and vCE )

It is typically derived as ),(

)(

CEBC

BEB

vi givfi

==

Simplified physical structure

BJT iv characteristics: iB = f(vBE) & iC = g(iB , vCE)


iB

Cut-off : BE is reverse biased

0 ,0 == CB ii

Active: BE is forward biased BC is reverse biased

BC ii β=

Saturation: BE is forward biased, BC is forward biased

1. Soft saturation: 2. Deep saturation: 3. Near cut-off:

BCCE iiv ,V 7.03.0 β≈≤≤

BCCE iiv ,V 3.01.0 β<≤≤0 ,V 1.0 ≈≤ CCE iv

Early Effect modifies iv characteristics in the active mode


iC is NOT constant in the active region.

Early Effect: Lines of iC vs vCE for different iB (or vBE ) coincide at vCE = − VA

+=

A

CEVvSC V

veIi TBE 1/

NPN BJT iv equations


“Linear” model

Cut-off : BE is reverse biased Active: BE is forward biased BC is reverse biased (Deep) Saturation: BE is forward biased BC is reverse biased

0 ,0 == CB ii0

0 ,0

DBE

CB

Vvii

<==

+=

==

A

CEVvSC

VvSCB

VveIi

eIii

TBE

TBE

1/

/

ββ0

0

, 0 ,

DCEBC

BDBE

VviiiVv

≥=≥=

β

BCsatCE

VvSB

iiVv

eIi TBE

,

/

ββ

<≈

=

BCsatCE

BDBE

iiVviVv

, 0 , 0

β<=≥=

V 2.0 ,V 7.0 Si,For 0 == satD VV

PNP transistor is the analog to NPN BJT


PNP transistor

Compared to a NPN: 1) Current directions are reversed 2) Voltage subscripts “switched”

“Linear” model

Cut-off : EB is reverse biased Active: EB is forward biased CB is reverse biased (Deep) Saturation: EB is forward biased CB is reverse biased

0 0 ,0

DEB

CB

Vvii

<==

0

0

, 0 ,

DECBC

BDEB

VviiiVv

≥=≥=

β

BCsatEC

BDEB

iiVviVv

, 0 , 0

β<=≥=

Notations


DC voltages: Use “Double subscript” of BJT terminal: VCC , VBB , VEE . Resistors:

Use “subscript” of BJT terminal: RC , RB , RE .

Voltage sources are identified by node voltage!

Transistor operates like a “valve:” iC & vCE are controlled by iB


Controller part: Circuit connected to BE sets iB

Controlled part: iC & vCE are set by transistor state (& outside circuit)

Cut-off (iB = 0): Valve Closed iC = 0

Active (iB > 0): Valve partially open iC = β iB

Saturation (iB > 0): Valve open iC < β iB iC limited by circuit connected to CE terminals, increasing iB does not increase iC

Recipe for solving BJT circuits (State of BJT is unknown before solving the circuit)

1. Write down BE-KVL and CE-KVL:

2. Assume BJT is OFF, Use BE-KVL to check: a. BJT OFF: Set iC = 0, use CE-KVL to find vCE (Done!) b. BJT ON: Compute iB

3. Assume BJT in active. Set iC = β iB . Use CE-KVL to find vCE . If vCE ≥ VD0 , Assumption Correct, otherwise in saturation:

4. BJT in Saturation. Set vCE = Vsat . Use CE-KVL to find iC . (Double-check iC < β iB )

NOTE: o For circuits with RE , both BE-KVL & CE-KVL have to be solved

simultaneously.



Example 1: Compute transistor parameters (Si BJT with β = 100).

CEC

BEB

vivi

+=

+×=

10 12 :KVL-CE

10 40 4 :KVL-BE3

3

incorrect Assumption V 7.0V 4V 4 0 10 40 4 :KVL-BE

V 7.0 and 0 :off-Cut Assume

0

30

→=>==→+××=

=<=

DBE

BEBE

DBEB

Vvvv

Vvi

0A 25.8 7.0 10 40 4 :KVL-BE

0 and V 7.0 :ON BE3

0

>=→+××=

≥==

µBB

BDBE

iiiVv

correct Assumption V 7.0V 75.3V 75.3 1025.8 10 12 :KVL-CE

mA 25.81025.8100

V 7.0 and :Active Assume

0

33

60

→=>==→+××=

=××==

=≥=

−

−

DCE

CECE

BC

DCEBC

Vvvv

iiVvii

β

β

BJT Transfer Function (1)


CECCCC

BEBBi

viRVviRv+=

+= :KVL-CE

:KVL-BE

0 :KVL-CE0

0 :KVL-BE and 0 :off-Cut 0

CCCECECCC

C

iBEBEBi

DBEB

VvvRVi

vvvRvVvi

=→+×==

=→+×=<=

,0 ,0 Cutoffin BJT For 0

CCCECB

Di

VviiVv

===→<

0

:KVL-BE

0 and :ON BE

0

00

0

DiB

B

DiBDBBi

BDBE

VviR

VviViRv

iVv

≥→≥

−=→+×=

≥=



CECCCC

B

DiBDBE

viRVR

VviVv

+=

−==

:KVL-CE

and :ON BE 00

BC

DCCDiDCE

CCCCCECECCCC

B

DiC

DCEBc

RRVVVvVv

iR-VvviRVR

Vvi

Vvii

/

:KVL-CE

and :Active

000

0

0

β

β

β

−+≤→≥

=→+=

−×=

≥=

activein BJT /

For 000 →

−+≤≤

BC

DCCDiD RR

VVVvVβ



CECCCC

B

DiBDBE

viRVR

VviVv

+=

−==

:KVL-CE

and :ON BE 00

BC

satCCDIHiBc

C

satCCCsatCCCC

BcsatCE

RRVVVVvii

RV-ViViRV

iiVv

/

:KVL-CE

and :nSaturaatio

0 ββ

β

−+=>→<

=→+=

<=

saturationin BJT /

For 00 →<

−+ i

BC

DCCD v

RRVVV

β



saturation deepin BJT /

activein BJT /

Cutoffin BJT

0

000

0

→<−

+

→−

+≤≤

→<

iBC

satCCD

BC

DCCDiD

Di

vRRVVV

RRVVVvV

Vv

β

β

BJT transfer function on the load line


CCCCCE iRVv )KVL-(CE Line Load

−=

togetherincrease & :Active 0

CB

IHiD

iiVvV ≤≤

unchanged but increases :Saturation

CB

iIH

iivV <

:offCut

0Di Vv <−

BJT as a switch

Use: Logic gate can turn loads ON (BJT in saturation) or OFF (BJT in cut-off)

ic is uniquely set by CE circuit (as vce = Vsat)

RB is chosen such that BJT is in deep saturation with a wide margin (e.g., iB = 0.2 ic /β)


Load is placed in collector circuit

*Lab 4 circuit Solved in Lecture notes (problems 12 & 13)

BJT as a Digital Gate

Other variants: Diode-transistor logic (DTL) and transistor-transistor logic (TTL) BJT logic gates are not used anymore except for high-speed emitter-coupled

logic circuits o Low speed (switching to saturation is quite slow). o Large space and power requirements on ICs


RTL NOT gate (VL = Vsat , VH = VCC)

Resistor-Transistor logic (RTL)

RTL NOR gate* RTL NAND gate*

*Solved in Lecture notes (problems 14 & 15)

BJT β varies substantially

Our BJT model includes three parameters: VD0 , Vsat and β o VD0 and Vsat depend on base semiconductor: o For Si, VD0 = 0.7 V, Vsat = 0.2 V

Transistor β depends on many factors: o Strongly depends on temperature (9% increase per oC) o Depends on iC (not constant as assumed in the model) o β of similarly manufactured BJT can vary (manufacturer spec sheet

typically gives a range as well as an average value for β ) o We will use the average β in calculations (PSpice also uses average β but

includes temperature and iC dependence). o βmin is an important parameter. For example, to ensure operation in

deep saturation for all similar model BJTs, we need to set iC /iB < βmin


Bipolar Junction Transistor (BJT)aries.ucsd.edu/.../ECE65/12-W/Slides/ECE65_W12-BJT.pdf · A BJT consists of three regions F. Najmabadi, ECE65, Winter 2012 Simplified physical structure.

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